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Crystallographical analysis of shear bands initiation and propagation in pure metals

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HAL Id: jpa-00245844

https://hal.archives-ouvertes.fr/jpa-00245844

Submitted on 1 Jan 1988

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Crystallographical analysis of shear bands initiation and propagation in pure metals

Ph. Dubois, C. Rey

To cite this version:

Ph. Dubois, C. Rey. Crystallographical analysis of shear bands initiation and propagation in pure metals. Revue de Physique Appliquée, Société française de physique / EDP, 1988, 23 (4), pp.696-696.

�10.1051/rphysap:01988002304069600�. �jpa-00245844�

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696

CRYSTALLOGRAPHICAL ANALYSIS OF SHEAR BANDS INITIATION AND PROPAGATION IN PURE METALS

Ph. DUBOIS and C. REY

LPMTM, Université PARIS-NORD - Av. J.B. Clément 93430 - VILLETANEUSE

Revue

Phys. Appl.

23

(1988)

696 AVRIL

1988,

Our purpose was to determine conditions of shear bands initiation and propagation in pure copper

single or polycrystals sollicited by tensile load and rolling.

Tensile tests were carried out "in situ" on single crystal oriented for double slip, thanks to a SEM.

So we were able to determine the crystallographi-

cal nature of shear planes for various tensile axis orientation. Four orientations closed to

|001|, |-1,1,3|, |-1,1,2|

and

|-1,1,1|

were

investigated. In all cases shear banding occured

in the necking area after a mean strain of about 55%. "In situ" observations pointed out that the localization mode was always caracterized by shearing in a very thin and planar band which width increased with increasing strain.

We had compared our experimental results to the prediction of the theoretical model developped by

Pierce

Ill

for rigid plastic materials. Founded upon Biot

(2I,

Hill and

Hutchinson 131

and Pierce Asaro and Needleman

|4|

works.-, It was assumed that

crystal plasticity was rate independent, governed by Schmid’s law, moreover the crystal was oriented

in double ship deformation for tensile loading.

For such a double orientation, a thin band of intense shearing limited by two nearly parallel planes grew in the crystal (fig.1). The transfor- mation gradient rate F was supposed to show an abrupt change of value in the thin band compared

to the bulk one.

According to different authors, the discontinuity

must be of the form :

where G and N were the shearing vector and the

unit normal to the band. Traction rates must be continuous across the shear planes, so one must

have :

where S was the nominal stress tensor.

The misfit between experimental observations and theoretical predictions about crystallographical

orientations of shear planes led us to introduce

in the model some other parameters in order to take into account :

- the tensile test direction

- the stress field induce by the neck

- conditions on the strain field compa- tibility.

Fig.1 Shear-band mode for tensile loa- ding.

By these formulation we defined "potential shear systems" and are studying some criterions in order to determine the more favorable systems.

In polycrystals case, strained by rolling, fidu-

cial grids were set down on the longitudinal section, in order to point out the displacement

induced by shear bands and to analyse the inter- action between shear bands and grain boundaries. A 1 MM2 square grid with 5 vm mesh size and an

average 0.5 um grid line was obtained by a photo-

resist technique, using the beam of a SEM. Our observations, pointed out that (Fig.2) :

- macroscopical shear bands were constituted of

microscopical ones

- shearing intensity was proportional to the

number of microscopical bands activated inside

macroscopical ones

- strain increased by elongation of initial shear bands and nucleation of new bands in the

vicinity of initial ones.

Previous works on rolled polycrystals have reported that shear bands appeared inside somme especially oriented grains. With intend to carac-

terize the conditions of initiation and propa- gation of such bands, experiments on special

oriented bicrystals have been undertaken.

REFERENCES

1 D. PEIRCE J. Mech. Phys. Solids 31 (1983) 133.

2 M.A. BIOT "Mechanics of Incremental Deforma-

tions", edited by Willey (1965).

3 R. HILL and J.W.. HUTCHINSON J. Mech. Phys.

Solids, 23 (1975) 239.

4 D. PEIRCE et al Acta Met. 30 (1982) 1087.

Fig.2 Propagation of shear band in rol- led polycrystals.

- Initial bands,...new bands.

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/rphysap:01988002304069600

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